Bump version to 0.4.0

Update raytracing mesh example to push mesh outside of photon shell

Patch bug where phi blows up on the horizon. Added a warning to indicate that this is happening. A proper fix would require regularizing the integral

Project.toml

@@ -1,7 +1,7 @@
 name = "Krang"
 uuid = "54806c32-d51a-438d-8447-e0041be2fbfb"
 authors = ["Dominic <[email protected]> and contributors"]
-version = "0.3.1"
+version = "0.4.0"
 
 [deps]
 DocStringExtensions = "ffbed154-4ef7-542d-bbb7-c09d3a79fcae"

examples/level-set-example.jl

@@ -1,4 +1,4 @@
-# # Raytracing a Level set geometry
+# # Raytracing a Level Set geometry
 # A level set geoemtry is defined by a constraint equations $f(x,y,z)=0$.
 # We will ray trace an example parabaloid geometry in this example as a simple geometric jet model.
 using Krang
@@ -19,15 +19,16 @@ struct Parabaloid{T} <: Krang.AbstractLevelSetGeometry{T}
     rh::T
     index::T
 end
-function (geometry::Parabaloid)(x,y,z)
-    r = sqrt(x^2+y^2+z^2)
-    return 1-(r/geometry.rh)^geometry.index*(1-z/r)
+function (geometry::Parabaloid)(x, y, z)
+    r = sqrt(x^2 + y^2 + z^2)
+    return 1 - (r / geometry.rh)^geometry.index * (1 - z / r)
 end
 
 # The jet will be emit a constant intensity whose physics we define in the `XMaterial`.
-# [!NOTE] We are ignoring relativistic effects in this example. 
+# > [!NOTE] 
+# > We are ignoring relativistic effects in this example. 
 struct XMaterial <: Krang.AbstractMaterial end
-function (mat::XMaterial)(pix, intersection) where T
+function (mat::XMaterial)(pix, intersection)
     return 1.0
 end
 
@@ -38,7 +39,7 @@ fig = GLMk.Figure();
 ax = GLMk.Axis(fig[1, 1], aspect = 1)
 
 
-intersections = raytrace(camera, Krang.Mesh(parabaloid, XMaterial()), res = 1_00)
+intersections = raytrace(camera, Krang.Mesh(parabaloid, XMaterial()), res = 1_00);
 
 # And plot the image with GLMakie, 
 

examples/mino-time-example.jl

@@ -45,7 +45,7 @@ camera = Krang.SlowLightIntensityCamera(metric, θo, -ρmax, ρmax, -ρmax, ρma
 # We will create a loop to plot the emission coordinates for each `τ` using the `emission_coordinates!` function.
 # Let us now create a figure to plot the emission coordinates on.
 
-fig = GLMk.Figure(resolution = (500, 600));
+fig = GLMk.Figure(size = (500, 600));
 
 
 recording =

examples/neural-net-example.jl

@@ -209,10 +209,7 @@ loss_function(pixels, target_img, ps_trained, st_trained)
 using Printf
 
 fig = Figure(size = (700, 300))
-heatmap!(
-    Axis(fig[1, 1], aspect = 1, title = "Target Image"),
-    reshape(target_img, sze, sze),
-)
+heatmap!(Axis(fig[1, 1], aspect = 1, title = "Target Image"), reshape(target_img, sze, sze))
 heatmap!(
     Axis(
         fig[1, 2],

examples/raytracing-mesh-example.jl

@@ -29,7 +29,7 @@ bunny_mesh = translate(
         0.0,
     ),
     2.0,
-    7.0,
+    10.0,
     -10.0,
 );
 
@@ -109,7 +109,12 @@ recording = GLMk.record(fig, "mesh.mp4", 1:sze*sze, framerate = 120) do i
     end
 
     cart_line = map(
-        x -> (x.rs * sin(x.θs) * cos(x.ϕs), x.rs * sin(x.θs) * sin(x.ϕs), x.rs * cos(x.θs)),
+        x -> Krang.boyer_lindquist_to_quasi_cartesian_kerr_schild_fast_light(
+            metric,
+            x.rs,
+            x.θs,
+            x.ϕs,
+        ),
         line,
     )
     GLMk.lines!(ax3, cart_line, color = :red)

src/schemes/RayTrace.jl

@@ -194,6 +194,11 @@ function ϕ_kerr_schild(metric::Kerr{T}, rBL, ϕBL) where {T}
 
     term1 = a / (2temp) * log(abs(num / den))
     term2 = -atan(a / rBL)
+    ans = ϕBL - term1 - term2
+    if isinf(ans)
+        @warn "ϕ_kerr_schild is inf at rs=$rBL. This usually happens if the ray intersects the horizon."
+        return ϕBL - term2
+    end
     return ϕBL - term1 - term2
 end